// This file is part of Eigen, a lightweight C++ template library // for linear algebra. // // Copyright (C) 2008-2010 Gael Guennebaud <gael.guennebaud@inria.fr> // Copyright (C) 2010 Jitse Niesen <jitse@maths.leeds.ac.uk> // // This Source Code Form is subject to the terms of the Mozilla // Public License v. 2.0. If a copy of the MPL was not distributed // with this file, You can obtain one at http://mozilla.org/MPL/2.0/.
/** \eigenvalues_module \ingroup Eigenvalues_Module * * * \class SelfAdjointEigenSolver * * \brief Computes eigenvalues and eigenvectors of selfadjoint matrices * * \tparam _MatrixType the type of the matrix of which we are computing the * eigendecomposition; this is expected to be an instantiation of the Matrix * class template. * * A matrix \f$ A \f$ is selfadjoint if it equals its adjoint. For real * matrices, this means that the matrix is symmetric: it equals its * transpose. This class computes the eigenvalues and eigenvectors of a * selfadjoint matrix. These are the scalars \f$ \lambda \f$ and vectors * \f$ v \f$ such that \f$ Av = \lambda v \f$. The eigenvalues of a * selfadjoint matrix are always real. If \f$ D \f$ is a diagonal matrix with * the eigenvalues on the diagonal, and \f$ V \f$ is a matrix with the * eigenvectors as its columns, then \f$ A = V D V^{-1} \f$. This is called the * eigendecomposition. * * For a selfadjoint matrix, \f$ V \f$ is unitary, meaning its inverse is equal * to its adjoint, \f$ V^{-1} = V^{\dagger} \f$. If \f$ A \f$ is real, then * \f$ V \f$ is also real and therefore orthogonal, meaning its inverse is * equal to its transpose, \f$ V^{-1} = V^T \f$. * * The algorithm exploits the fact that the matrix is selfadjoint, making it * faster and more accurate than the general purpose eigenvalue algorithms * implemented in EigenSolver and ComplexEigenSolver. * * Only the \b lower \b triangular \b part of the input matrix is referenced. * * Call the function compute() to compute the eigenvalues and eigenvectors of * a given matrix. Alternatively, you can use the * SelfAdjointEigenSolver(const MatrixType&, int) constructor which computes * the eigenvalues and eigenvectors at construction time. Once the eigenvalue * and eigenvectors are computed, they can be retrieved with the eigenvalues() * and eigenvectors() functions. * * The documentation for SelfAdjointEigenSolver(const MatrixType&, int) * contains an example of the typical use of this class. * * To solve the \em generalized eigenvalue problem \f$ Av = \lambda Bv \f$ and * the likes, see the class GeneralizedSelfAdjointEigenSolver. * * \sa MatrixBase::eigenvalues(), class EigenSolver, class ComplexEigenSolver
*/ template<typename _MatrixType> class SelfAdjointEigenSolver
{ public:
/** \brief Scalar type for matrices of type \p _MatrixType. */ typedeftypename MatrixType::Scalar Scalar; typedef Eigen::Index Index; ///< \deprecated since Eigen 3.3
/** \brief Real scalar type for \p _MatrixType. * * This is just \c Scalar if #Scalar is real (e.g., \c float or * \c double), and the type of the real part of \c Scalar if #Scalar is * complex.
*/ typedeftypename NumTraits<Scalar>::Real RealScalar;
/** \brief Type for vector of eigenvalues as returned by eigenvalues(). * * This is a column vector with entries of type #RealScalar. * The length of the vector is the size of \p _MatrixType.
*/ typedeftypename internal::plain_col_type<MatrixType, RealScalar>::type RealVectorType; typedef Tridiagonalization<MatrixType> TridiagonalizationType; typedeftypename TridiagonalizationType::SubDiagonalType SubDiagonalType;
/** \brief Default constructor for fixed-size matrices. * * The default constructor is useful in cases in which the user intends to * perform decompositions via compute(). This constructor * can only be used if \p _MatrixType is a fixed-size matrix; use * SelfAdjointEigenSolver(Index) for dynamic-size matrices. * * Example: \include SelfAdjointEigenSolver_SelfAdjointEigenSolver.cpp * Output: \verbinclude SelfAdjointEigenSolver_SelfAdjointEigenSolver.out
*/
EIGEN_DEVICE_FUNC
SelfAdjointEigenSolver()
: m_eivec(),
m_eivalues(),
m_subdiag(),
m_hcoeffs(),
m_info(InvalidInput),
m_isInitialized(false),
m_eigenvectorsOk(false)
{ }
/** \brief Constructor, pre-allocates memory for dynamic-size matrices. * * \param [in] size Positive integer, size of the matrix whose * eigenvalues and eigenvectors will be computed. * * This constructor is useful for dynamic-size matrices, when the user * intends to perform decompositions via compute(). The \p size * parameter is only used as a hint. It is not an error to give a wrong * \p size, but it may impair performance. * * \sa compute() for an example
*/
EIGEN_DEVICE_FUNC explicit SelfAdjointEigenSolver(Index size)
: m_eivec(size, size),
m_eivalues(size),
m_subdiag(size > 1 ? size - 1 : 1),
m_hcoeffs(size > 1 ? size - 1 : 1),
m_isInitialized(false),
m_eigenvectorsOk(false)
{}
/** \brief Constructor; computes eigendecomposition of given matrix. * * \param[in] matrix Selfadjoint matrix whose eigendecomposition is to * be computed. Only the lower triangular part of the matrix is referenced. * \param[in] options Can be #ComputeEigenvectors (default) or #EigenvaluesOnly. * * This constructor calls compute(const MatrixType&, int) to compute the * eigenvalues of the matrix \p matrix. The eigenvectors are computed if * \p options equals #ComputeEigenvectors. * * Example: \include SelfAdjointEigenSolver_SelfAdjointEigenSolver_MatrixType.cpp * Output: \verbinclude SelfAdjointEigenSolver_SelfAdjointEigenSolver_MatrixType.out * * \sa compute(const MatrixType&, int)
*/ template<typename InputType>
EIGEN_DEVICE_FUNC explicit SelfAdjointEigenSolver(const EigenBase<InputType>& matrix, int options = ComputeEigenvectors)
: m_eivec(matrix.rows(), matrix.cols()),
m_eivalues(matrix.cols()),
m_subdiag(matrix.rows() > 1 ? matrix.rows() - 1 : 1),
m_hcoeffs(matrix.cols() > 1 ? matrix.cols() - 1 : 1),
m_isInitialized(false),
m_eigenvectorsOk(false)
{
compute(matrix.derived(), options);
}
/** \brief Computes eigendecomposition of given matrix. * * \param[in] matrix Selfadjoint matrix whose eigendecomposition is to * be computed. Only the lower triangular part of the matrix is referenced. * \param[in] options Can be #ComputeEigenvectors (default) or #EigenvaluesOnly. * \returns Reference to \c *this * * This function computes the eigenvalues of \p matrix. The eigenvalues() * function can be used to retrieve them. If \p options equals #ComputeEigenvectors, * then the eigenvectors are also computed and can be retrieved by * calling eigenvectors(). * * This implementation uses a symmetric QR algorithm. The matrix is first * reduced to tridiagonal form using the Tridiagonalization class. The * tridiagonal matrix is then brought to diagonal form with implicit * symmetric QR steps with Wilkinson shift. Details can be found in * Section 8.3 of Golub \& Van Loan, <i>%Matrix Computations</i>. * * The cost of the computation is about \f$ 9n^3 \f$ if the eigenvectors * are required and \f$ 4n^3/3 \f$ if they are not required. * * This method reuses the memory in the SelfAdjointEigenSolver object that * was allocated when the object was constructed, if the size of the * matrix does not change. * * Example: \include SelfAdjointEigenSolver_compute_MatrixType.cpp * Output: \verbinclude SelfAdjointEigenSolver_compute_MatrixType.out * * \sa SelfAdjointEigenSolver(const MatrixType&, int)
*/ template<typename InputType>
EIGEN_DEVICE_FUNC
SelfAdjointEigenSolver& compute(const EigenBase<InputType>& matrix, int options = ComputeEigenvectors);
/** \brief Computes eigendecomposition of given matrix using a closed-form algorithm * * This is a variant of compute(const MatrixType&, int options) which * directly solves the underlying polynomial equation. * * Currently only 2x2 and 3x3 matrices for which the sizes are known at compile time are supported (e.g., Matrix3d). * * This method is usually significantly faster than the QR iterative algorithm * but it might also be less accurate. It is also worth noting that * for 3x3 matrices it involves trigonometric operations which are * not necessarily available for all scalar types. * * For the 3x3 case, we observed the following worst case relative error regarding the eigenvalues: * - double: 1e-8 * - float: 1e-3 * * \sa compute(const MatrixType&, int options)
*/
EIGEN_DEVICE_FUNC
SelfAdjointEigenSolver& computeDirect(const MatrixType& matrix, int options = ComputeEigenvectors);
/** *\brief Computes the eigen decomposition from a tridiagonal symmetric matrix * * \param[in] diag The vector containing the diagonal of the matrix. * \param[in] subdiag The subdiagonal of the matrix. * \param[in] options Can be #ComputeEigenvectors (default) or #EigenvaluesOnly. * \returns Reference to \c *this * * This function assumes that the matrix has been reduced to tridiagonal form. * * \sa compute(const MatrixType&, int) for more information
*/
SelfAdjointEigenSolver& computeFromTridiagonal(const RealVectorType& diag, const SubDiagonalType& subdiag , int options=ComputeEigenvectors);
/** \brief Returns the eigenvectors of given matrix. * * \returns A const reference to the matrix whose columns are the eigenvectors. * * \pre The eigenvectors have been computed before. * * Column \f$ k \f$ of the returned matrix is an eigenvector corresponding * to eigenvalue number \f$ k \f$ as returned by eigenvalues(). The * eigenvectors are normalized to have (Euclidean) norm equal to one. If * this object was used to solve the eigenproblem for the selfadjoint * matrix \f$ A \f$, then the matrix returned by this function is the * matrix \f$ V \f$ in the eigendecomposition \f$ A = V D V^{-1} \f$. * * For a selfadjoint matrix, \f$ V \f$ is unitary, meaning its inverse is equal * to its adjoint, \f$ V^{-1} = V^{\dagger} \f$. If \f$ A \f$ is real, then * \f$ V \f$ is also real and therefore orthogonal, meaning its inverse is * equal to its transpose, \f$ V^{-1} = V^T \f$. * * Example: \include SelfAdjointEigenSolver_eigenvectors.cpp * Output: \verbinclude SelfAdjointEigenSolver_eigenvectors.out * * \sa eigenvalues()
*/
EIGEN_DEVICE_FUNC const EigenvectorsType& eigenvectors() const
{
eigen_assert(m_isInitialized && "SelfAdjointEigenSolver is not initialized.");
eigen_assert(m_eigenvectorsOk && "The eigenvectors have not been computed together with the eigenvalues."); return m_eivec;
}
/** \brief Returns the eigenvalues of given matrix. * * \returns A const reference to the column vector containing the eigenvalues. * * \pre The eigenvalues have been computed before. * * The eigenvalues are repeated according to their algebraic multiplicity, * so there are as many eigenvalues as rows in the matrix. The eigenvalues * are sorted in increasing order. * * Example: \include SelfAdjointEigenSolver_eigenvalues.cpp * Output: \verbinclude SelfAdjointEigenSolver_eigenvalues.out * * \sa eigenvectors(), MatrixBase::eigenvalues()
*/
EIGEN_DEVICE_FUNC const RealVectorType& eigenvalues() const
{
eigen_assert(m_isInitialized && "SelfAdjointEigenSolver is not initialized."); return m_eivalues;
}
/** \brief Computes the positive-definite square root of the matrix. * * \returns the positive-definite square root of the matrix * * \pre The eigenvalues and eigenvectors of a positive-definite matrix * have been computed before. * * The square root of a positive-definite matrix \f$ A \f$ is the * positive-definite matrix whose square equals \f$ A \f$. This function * uses the eigendecomposition \f$ A = V D V^{-1} \f$ to compute the * square root as \f$ A^{1/2} = V D^{1/2} V^{-1} \f$. * * Example: \include SelfAdjointEigenSolver_operatorSqrt.cpp * Output: \verbinclude SelfAdjointEigenSolver_operatorSqrt.out * * \sa operatorInverseSqrt(), <a href="unsupported/group__MatrixFunctions__Module.html">MatrixFunctions Module</a>
*/
EIGEN_DEVICE_FUNC
MatrixType operatorSqrt() const
{
eigen_assert(m_isInitialized && "SelfAdjointEigenSolver is not initialized.");
eigen_assert(m_eigenvectorsOk && "The eigenvectors have not been computed together with the eigenvalues."); return m_eivec * m_eivalues.cwiseSqrt().asDiagonal() * m_eivec.adjoint();
}
/** \brief Computes the inverse square root of the matrix. * * \returns the inverse positive-definite square root of the matrix * * \pre The eigenvalues and eigenvectors of a positive-definite matrix * have been computed before. * * This function uses the eigendecomposition \f$ A = V D V^{-1} \f$ to * compute the inverse square root as \f$ V D^{-1/2} V^{-1} \f$. This is * cheaper than first computing the square root with operatorSqrt() and * then its inverse with MatrixBase::inverse(). * * Example: \include SelfAdjointEigenSolver_operatorInverseSqrt.cpp * Output: \verbinclude SelfAdjointEigenSolver_operatorInverseSqrt.out * * \sa operatorSqrt(), MatrixBase::inverse(), <a href="unsupported/group__MatrixFunctions__Module.html">MatrixFunctions Module</a>
*/
EIGEN_DEVICE_FUNC
MatrixType operatorInverseSqrt() const
{
eigen_assert(m_isInitialized && "SelfAdjointEigenSolver is not initialized.");
eigen_assert(m_eigenvectorsOk && "The eigenvectors have not been computed together with the eigenvalues."); return m_eivec * m_eivalues.cwiseInverse().cwiseSqrt().asDiagonal() * m_eivec.adjoint();
}
/** \brief Reports whether previous computation was successful. * * \returns \c Success if computation was successful, \c NoConvergence otherwise.
*/
EIGEN_DEVICE_FUNC
ComputationInfo info() const
{
eigen_assert(m_isInitialized && "SelfAdjointEigenSolver is not initialized."); return m_info;
}
/** \brief Maximum number of iterations. * * The algorithm terminates if it does not converge within m_maxIterations * n iterations, where n * denotes the size of the matrix. This value is currently set to 30 (copied from LAPACK).
*/ staticconstint m_maxIterations = 30;
namespace internal { /** \internal * * \eigenvalues_module \ingroup Eigenvalues_Module * * Performs a QR step on a tridiagonal symmetric matrix represented as a * pair of two vectors \a diag and \a subdiag. * * \param diag the diagonal part of the input selfadjoint tridiagonal matrix * \param subdiag the sub-diagonal part of the input selfadjoint tridiagonal matrix * \param start starting index of the submatrix to work on * \param end last+1 index of the submatrix to work on * \param matrixQ pointer to the column-major matrix holding the eigenvectors, can be 0 * \param n size of the input matrix * * For compilation efficiency reasons, this procedure does not use eigen expression * for its arguments. * * Implemented from Golub's "Matrix Computations", algorithm 8.3.2: * "implicit symmetric QR step with Wilkinson shift"
*/ template<int StorageOrder,typename RealScalar, typename Scalar, typename Index>
EIGEN_DEVICE_FUNC staticvoid tridiagonal_qr_step(RealScalar* diag, RealScalar* subdiag, Index start, Index end, Scalar* matrixQ, Index n);
}
namespace internal { /** * \internal * \brief Compute the eigendecomposition from a tridiagonal matrix * * \param[in,out] diag : On input, the diagonal of the matrix, on output the eigenvalues * \param[in,out] subdiag : The subdiagonal part of the matrix (entries are modified during the decomposition) * \param[in] maxIterations : the maximum number of iterations * \param[in] computeEigenvectors : whether the eigenvectors have to be computed or not * \param[out] eivec : The matrix to store the eigenvectors if computeEigenvectors==true. Must be allocated on input. * \returns \c Success or \c NoConvergence
*/ template<typename MatrixType, typename DiagType, typename SubDiagType>
EIGEN_DEVICE_FUNC
ComputationInfo computeFromTridiagonal_impl(DiagType& diag, SubDiagType& subdiag, const Index maxIterations, bool computeEigenvectors, MatrixType& eivec)
{
ComputationInfo info; typedeftypename MatrixType::Scalar Scalar;
Index n = diag.size();
Index end = n-1;
Index start = 0;
Index iter = 0; // total number of iterations
// find the largest unreduced block at the end of the matrix. while (end>0 && subdiag[end-1]==RealScalar(0))
{
end--;
} if (end<=0) break;
// if we spent too many iterations, we give up
iter++; if(iter > maxIterations * n) break;
start = end - 1; while (start>0 && subdiag[start-1]!=0)
start--;
internal::tridiagonal_qr_step<MatrixType::Flags&RowMajorBit ? RowMajor : ColMajor>(diag.data(), subdiag.data(), start, end, computeEigenvectors ? eivec.data() : (Scalar*)0, n);
} if (iter <= maxIterations * n)
info = Success; else
info = NoConvergence;
// Sort eigenvalues and corresponding vectors. // TODO make the sort optional ? // TODO use a better sort algorithm !! if (info == Success)
{ for (Index i = 0; i < n-1; ++i)
{
Index k;
diag.segment(i,n-i).minCoeff(&k); if (k > 0)
{
numext::swap(diag[i], diag[k+i]); if(computeEigenvectors)
eivec.col(i).swap(eivec.col(k+i));
}
}
} return info;
}
template<typename SolverType,int Size,bool IsComplex> struct direct_selfadjoint_eigenvalues
{
EIGEN_DEVICE_FUNC staticinlinevoid run(SolverType& eig, consttypename SolverType::MatrixType& A, int options)
{ eig.compute(A,options); }
};
/** \internal * Computes the roots of the characteristic polynomial of \a m. * For numerical stability m.trace() should be near zero and to avoid over- or underflow m should be normalized.
*/
EIGEN_DEVICE_FUNC staticinlinevoid computeRoots(const MatrixType& m, VectorType& roots)
{
EIGEN_USING_STD(sqrt)
EIGEN_USING_STD(atan2)
EIGEN_USING_STD(cos)
EIGEN_USING_STD(sin) const Scalar s_inv3 = Scalar(1)/Scalar(3); const Scalar s_sqrt3 = sqrt(Scalar(3));
// The characteristic equation is x^3 - c2*x^2 + c1*x - c0 = 0. The // eigenvalues are the roots to this equation, all guaranteed to be // real-valued, because the matrix is symmetric.
Scalar c0 = m(0,0)*m(1,1)*m(2,2) + Scalar(2)*m(1,0)*m(2,0)*m(2,1) - m(0,0)*m(2,1)*m(2,1) - m(1,1)*m(2,0)*m(2,0) - m(2,2)*m(1,0)*m(1,0);
Scalar c1 = m(0,0)*m(1,1) - m(1,0)*m(1,0) + m(0,0)*m(2,2) - m(2,0)*m(2,0) + m(1,1)*m(2,2) - m(2,1)*m(2,1);
Scalar c2 = m(0,0) + m(1,1) + m(2,2);
// Construct the parameters used in classifying the roots of the equation // and in solving the equation for the roots in closed form.
Scalar c2_over_3 = c2*s_inv3;
Scalar a_over_3 = (c2*c2_over_3 - c1)*s_inv3;
a_over_3 = numext::maxi(a_over_3, Scalar(0));
// Compute the eigenvalues by solving for the roots of the polynomial.
Scalar rho = sqrt(a_over_3);
Scalar theta = atan2(sqrt(q),half_b)*s_inv3; // since sqrt(q) > 0, atan2 is in [0, pi] and theta is in [0, pi/3]
Scalar cos_theta = cos(theta);
Scalar sin_theta = sin(theta); // roots are already sorted, since cos is monotonically decreasing on [0, pi]
roots(0) = c2_over_3 - rho*(cos_theta + s_sqrt3*sin_theta); // == 2*rho*cos(theta+2pi/3)
roots(1) = c2_over_3 - rho*(cos_theta - s_sqrt3*sin_theta); // == 2*rho*cos(theta+ pi/3)
roots(2) = c2_over_3 + Scalar(2)*rho*cos_theta;
}
EIGEN_DEVICE_FUNC staticinlinebool extract_kernel(MatrixType& mat, Ref<VectorType> res, Ref<VectorType> representative)
{
EIGEN_USING_STD(abs);
EIGEN_USING_STD(sqrt);
Index i0; // Find non-zero column i0 (by construction, there must exist a non zero coefficient on the diagonal):
mat.diagonal().cwiseAbs().maxCoeff(&i0); // mat.col(i0) is a good candidate for an orthogonal vector to the current eigenvector, // so let's save it:
representative = mat.col(i0);
Scalar n0, n1;
VectorType c0, c1;
n0 = (c0 = representative.cross(mat.col((i0+1)%3))).squaredNorm();
n1 = (c1 = representative.cross(mat.col((i0+2)%3))).squaredNorm(); if(n0>n1) res = c0/sqrt(n0); else res = c1/sqrt(n1);
// Shift the matrix to the mean eigenvalue and map the matrix coefficients to [-1:1] to avoid over- and underflow.
Scalar shift = mat.trace() / Scalar(3); // TODO Avoid this copy. Currently it is necessary to suppress bogus values when determining maxCoeff and for computing the eigenvectors later
MatrixType scaledMat = mat.template selfadjointView<Lower>();
scaledMat.diagonal().array() -= shift;
Scalar scale = scaledMat.cwiseAbs().maxCoeff(); if(scale > 0) scaledMat /= scale; // TODO for scale==0 we could save the remaining operations
// compute the eigenvalues
computeRoots(scaledMat,eivals);
// compute the eigenvectors if(computeEigenvectors)
{ if((eivals(2)-eivals(0))<=Eigen::NumTraits<Scalar>::epsilon())
{ // All three eigenvalues are numerically the same
eivecs.setIdentity();
} else
{
MatrixType tmp;
tmp = scaledMat;
// Compute the eigenvector of the most distinct eigenvalue
Scalar d0 = eivals(2) - eivals(1);
Scalar d1 = eivals(1) - eivals(0);
Index k(0), l(2); if(d0 > d1)
{
numext::swap(k,l);
d0 = d1;
}
// Compute the eigenvector of index k
{
tmp.diagonal().array () -= eivals(k); // By construction, 'tmp' is of rank 2, and its kernel corresponds to the respective eigenvector.
extract_kernel(tmp, eivecs.col(k), eivecs.col(l));
}
// Compute eigenvector of index l if(d0<=2*Eigen::NumTraits<Scalar>::epsilon()*d1)
{ // If d0 is too small, then the two other eigenvalues are numerically the same, // and thus we only have to ortho-normalize the near orthogonal vector we saved above.
eivecs.col(l) -= eivecs.col(k).dot(eivecs.col(l))*eivecs.col(l);
eivecs.col(l).normalize();
} else
{
tmp = scaledMat;
tmp.diagonal().array () -= eivals(l);
// Francis implicit QR step. template<int StorageOrder,typename RealScalar, typename Scalar, typename Index>
EIGEN_DEVICE_FUNC staticvoid tridiagonal_qr_step(RealScalar* diag, RealScalar* subdiag, Index start, Index end, Scalar* matrixQ, Index n)
{ // Wilkinson Shift.
RealScalar td = (diag[end-1] - diag[end])*RealScalar(0.5);
RealScalar e = subdiag[end-1]; // Note that thanks to scaling, e^2 or td^2 cannot overflow, however they can still // underflow thus leading to inf/NaN values when using the following commented code: // RealScalar e2 = numext::abs2(subdiag[end-1]); // RealScalar mu = diag[end] - e2 / (td + (td>0 ? 1 : -1) * sqrt(td*td + e2)); // This explain the following, somewhat more complicated, version:
RealScalar mu = diag[end]; if(td==RealScalar(0)) {
mu -= numext::abs(e);
} elseif (e != RealScalar(0)) { const RealScalar e2 = numext::abs2(e); const RealScalar h = numext::hypot(td,e); if(e2 == RealScalar(0)) {
mu -= e / ((td + (td>RealScalar(0) ? h : -h)) / e);
} else {
mu -= e2 / (td + (td>RealScalar(0) ? h : -h));
}
}
RealScalar x = diag[start] - mu;
RealScalar z = subdiag[start]; // If z ever becomes zero, the Givens rotation will be the identity and // z will stay zero for all future iterations. for (Index k = start; k < end && z != RealScalar(0); ++k)
{
JacobiRotation<RealScalar> rot;
rot.makeGivens(x, z);
// do T = G' T G
RealScalar sdk = rot.s() * diag[k] + rot.c() * subdiag[k];
RealScalar dkp1 = rot.s() * subdiag[k] + rot.c() * diag[k+1];
// "Chasing the bulge" to return to triangular form.
x = subdiag[k]; if (k < end - 1)
{
z = -rot.s() * subdiag[k+1];
subdiag[k + 1] = rot.c() * subdiag[k+1];
}
// apply the givens rotation to the unit matrix Q = Q * G if (matrixQ)
{ // FIXME if StorageOrder == RowMajor this operation is not very efficient
Map<Matrix<Scalar,Dynamic,Dynamic,StorageOrder> > q(matrixQ,n,n);
q.applyOnTheRight(k,k+1,rot);
}
}
}
} // end namespace internal
} // end namespace Eigen
#endif// EIGEN_SELFADJOINTEIGENSOLVER_H
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